Abstract
Any change with time in the state of a quantum mechanical system can be described by keeping the axes fixed and allowing the state vector to rotate, or by keeping the state vector fixed and allowing the axes to rotate. The two possibilities described above are called Schrödinger and Heisenberg picture, respectively. Let Ĥ be the Hamilton operator of the system. We assume that the Hamilton operator is self-adjoint.
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© 1998 Springer Science+Business Media Dordrecht
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Steeb, WH. (1998). Interaction Picture. In: Hilbert Spaces, Wavelets, Generalised Functions and Modern Quantum Mechanics. Mathematics and Its Applications, vol 451. Springer, Dordrecht. https://doi.org/10.1007/978-94-011-5332-4_7
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DOI: https://doi.org/10.1007/978-94-011-5332-4_7
Publisher Name: Springer, Dordrecht
Print ISBN: 978-94-010-6241-1
Online ISBN: 978-94-011-5332-4
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